<p>We introduce an Allen–Cahn type functional, <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {BE}_{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>BE</mtext> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation>, that defines an energy on separating hypersurfaces, <i>Y</i>, of closed Riemannian Manifolds. We establish <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="12" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>-convergence of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {BE}_{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>BE</mtext> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> to the area functional, and compute first and second variations of this functional under hypersurface perturbations. We then compute an explicit expansion for the variational formula as <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="44" /> </InlineMediaObject> <EquationSource Format="TEX">\(\varepsilon \rightarrow 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ε</mi> <mo stretchy="false">→</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. A key component of this proof is the invertibility of the linearized Allen–Cahn equation about a solution, on the space of functions vanishing on <i>Y</i>. We also relate the index and nullity of <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(\text {BE}_{\varepsilon }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>BE</mtext> <mi>ε</mi> </msub> </math></EquationSource> </InlineEquation> to the Allen–Cahn index and nullity of a corresponding solution vanishing on <i>Y</i>. We apply the second variation formula and index theorems to show that the family of 2<i>p</i>-dihedrally symmetric solutions to Allen–Cahn on <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(S^1\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>S</mi> <mn>1</mn> </msup> </math></EquationSource> </InlineEquation> have index <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="526_2025_3016_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(2p - 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>2</mn> <mi>p</mi> <mo>-</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and nullity 1.</p>

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Geometric variations of an Allen–Cahn energy on hypersurfaces

  • Jared Marx-Kuo,
  • Érico Melo Silva

摘要

We introduce an Allen–Cahn type functional, \(\text {BE}_{\varepsilon }\) BE ε , that defines an energy on separating hypersurfaces, Y, of closed Riemannian Manifolds. We establish \(\Gamma \) Γ -convergence of \(\text {BE}_{\varepsilon }\) BE ε to the area functional, and compute first and second variations of this functional under hypersurface perturbations. We then compute an explicit expansion for the variational formula as \(\varepsilon \rightarrow 0\) ε 0 . A key component of this proof is the invertibility of the linearized Allen–Cahn equation about a solution, on the space of functions vanishing on Y. We also relate the index and nullity of \(\text {BE}_{\varepsilon }\) BE ε to the Allen–Cahn index and nullity of a corresponding solution vanishing on Y. We apply the second variation formula and index theorems to show that the family of 2p-dihedrally symmetric solutions to Allen–Cahn on \(S^1\) S 1 have index \(2p - 1\) 2 p - 1 and nullity 1.